Causality and Relativity in Quantum Physics
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Introduction to Dynamical Triangulations
Introduction to Dynamical Triangulations Andrzej G¨orlich Niels Bohr Institute, University of Copenhagen Naxos, September 12th, 2011 Andrzej G¨orlich Causal Dynamical Triangulation Outline 1 Path integral for quantum gravity 2 Causal Dynamical Triangulations 3 Numerical setup 4 Phase diagram 5 Background geometry 6 Quantum fluctuations Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum mechanics A classical particle follows a unique trajectory. Quantum mechanics can be described by Path Integrals: All possible trajectories contribute to the transition amplitude. To define the functional integral, we discretize the time coordinate and approximate each path by linear pieces. quantum trajectory space classical trajectory t1 time t2 Andrzej G¨orlich Causal Dynamical Triangulation Path integral formulation of quantum gravity General Relativity: gravity is encoded in space-time geometry. The role of a trajectory plays now the geometry of four-dimensional space-time. All space-time histories contribute to the transition amplitude. -
Causality and Determinism: Tension, Or Outright Conflict?
1 Causality and Determinism: Tension, or Outright Conflict? Carl Hoefer ICREA and Universidad Autònoma de Barcelona Draft October 2004 Abstract: In the philosophical tradition, the notions of determinism and causality are strongly linked: it is assumed that in a world of deterministic laws, causality may be said to reign supreme; and in any world where the causality is strong enough, determinism must hold. I will show that these alleged linkages are based on mistakes, and in fact get things almost completely wrong. In a deterministic world that is anything like ours, there is no room for genuine causation. Though there may be stable enough macro-level regularities to serve the purposes of human agents, the sense of “causality” that can be maintained is one that will at best satisfy Humeans and pragmatists, not causal fundamentalists. Introduction. There has been a strong tendency in the philosophical literature to conflate determinism and causality, or at the very least, to see the former as a particularly strong form of the latter. The tendency persists even today. When the editors of the Stanford Encyclopedia of Philosophy asked me to write the entry on determinism, I found that the title was to be “Causal determinism”.1 I therefore felt obliged to point out in the opening paragraph that determinism actually has little or nothing to do with causation; for the philosophical tradition has it all wrong. What I hope to show in this paper is that, in fact, in a complex world such as the one we inhabit, determinism and genuine causality are probably incompatible with each other. -
Causality in Quantum Field Theory with Classical Sources
Causality in Quantum Field Theory with Classical Sources Bo-Sture K. Skagerstam1;a), Karl-Erik Eriksson2;b), Per K. Rekdal3;c) a)Department of Physics, NTNU, Norwegian University of Science and Technology, N-7491 Trondheim, Norway b) Department of Space, Earth and Environment, Chalmers University of Technology, SE-412 96 G¨oteborg, Sweden c)Molde University College, P.O. Box 2110, N-6402 Molde, Norway Abstract In an exact quantum-mechanical framework we show that space-time expectation values of the second-quantized electromagnetic fields in the Coulomb gauge, in the presence of a classical source, automatically lead to causal and properly retarded elec- tromagnetic field strengths. The classical ~-independent and gauge invariant Maxwell's equations then naturally emerge and are therefore also consistent with the classical spe- cial theory of relativity. The fundamental difference between interference phenomena due to the linear nature of the classical Maxwell theory as considered in, e.g., classical optics, and interference effects of quantum states is clarified. In addition to these is- sues, the framework outlined also provides for a simple approach to invariance under time-reversal, some spontaneous photon emission and/or absorption processes as well as an approach to Vavilov-Cherenkovˇ radiation. The inherent and necessary quan- tum uncertainty, limiting a precise space-time knowledge of expectation values of the quantum fields considered, is, finally, recalled. arXiv:1801.09947v2 [quant-ph] 30 Mar 2019 1Corresponding author. Email address: [email protected] 2Email address: [email protected] 3Email address: [email protected] 1. Introduction The roles of causality and retardation in classical and quantum-mechanical versions of electrodynamics are issues that one encounters in various contexts (for recent discussions see, e.g., Refs.[1]-[14]). -
Time and Causality in General Relativity
Time and Causality in General Relativity Ettore Minguzzi Universit`aDegli Studi Di Firenze FQXi International Conference. Ponta Delgada, July 10, 2009 FQXi Conference 2009, Ponta Delgada Time and Causality in General Relativity 1/8 Light cone A tangent vector v 2 TM is timelike, lightlike, causal or spacelike if g(v; v) <; =; ≤; > 0 respectively. Time orientation and spacetime At every point there are two cones of timelike vectors. The Lorentzian manifold is time orientable if a continuous choice of one of the cones, termed future, can be made. If such a choice has been made the Lorentzian manifold is time oriented and is also called spacetime. Lorentzian manifolds and light cones Lorentzian manifolds A Lorentzian manifold is a Hausdorff manifold M, of dimension n ≥ 2, endowed with a Lorentzian metric, that is a section g of T ∗M ⊗ T ∗M with signature (−; +;:::; +). FQXi Conference 2009, Ponta Delgada Time and Causality in General Relativity 2/8 Time orientation and spacetime At every point there are two cones of timelike vectors. The Lorentzian manifold is time orientable if a continuous choice of one of the cones, termed future, can be made. If such a choice has been made the Lorentzian manifold is time oriented and is also called spacetime. Lorentzian manifolds and light cones Lorentzian manifolds A Lorentzian manifold is a Hausdorff manifold M, of dimension n ≥ 2, endowed with a Lorentzian metric, that is a section g of T ∗M ⊗ T ∗M with signature (−; +;:::; +). Light cone A tangent vector v 2 TM is timelike, lightlike, causal or spacelike if g(v; v) <; =; ≤; > 0 respectively. -
Observation of Quantum Jumps in a Single Atom
VoLUME 57, NUMBER 14 PHYSICAL REVIEW LETTERS 6 OcTosER 1986 Observation of Quantum Jumps in a Single Atom J. C. Bergquist, Randall G. Hulet, Wayne M. Itano, and D. J. Wineland Time and Frequency Division, Jtiational Bureau ofStandards, Boulder, Colorado 80303 (Received 23 June 1986) %e detect the radiatively driven electric quadrupole transition to the metastable Dsy2 state in a single, laser-cooled Hg D ion by monitoring the abrupt cessation of the fluorescence signal from the laser-excited 'Si/2 Pi~2 first resonance line. %hen the ion "jumps" back from the metastable D state to the ground S state, the S P resonance fluorescence signal immediately returns. The sta- tistical properties of the quantum jumps are investigated; for example, photon antibunching in the emission from the D state is observed ~ith 100% efficiency. PACS numbers: 32.80,Pj, 42.SO.Dv Recently, a few laboratories have trapped and radia- ground state to the 5d 6s D5/2 state near 281.5 nm. tively cooled single atoms' 4 enabling a number of The lifetime of the metastable D state has recently unique experiments to be performed. One of the ex- been measured to be about 0.1 s.'5'6 A laser tuned periments now possible is to observe the "quantum just below resonance on the highly allowed S.P transi- jumps" to and from a metastable state in a single atom tion will cool the ion and, in our case, scatter up to by monitoring of the resonance fluorescence of a 5&&10~ photons/s. By collecting even a small fraction strong transition in which at least one of the states is of the scattered photons, we can easily monitor the coupled to the metastable state. -
Causality in the Quantum World
VIEWPOINT Causality in the Quantum World A new model extends the definition of causality to quantum-mechanical systems. by Jacques Pienaar∗ athematical models for deducing cause-effect relationships from statistical data have been successful in diverse areas of science (see Ref. [1] and references therein). Such models can Mbe applied, for instance, to establish causal relationships between smoking and cancer or to analyze risks in con- struction projects. Can similar models be extended to the microscopic world governed by the laws of quantum me- chanics? Answering this question could lead to advances in quantum information and to a better understanding of the foundations of quantum mechanics. Developing quantum Figure 1: In statistics, causal models can be used to extract extensions of causal models, however, has proven challeng- cause-effect relationships from empirical data on a complex ing because of the peculiar features of quantum mechanics. system. Existing models, however, do not apply if at least one For instance, if two or more quantum systems are entangled, component of the system (Y) is quantum. Allen et al. have now it is hard to deduce whether statistical correlations between proposed a quantum extension of causal models. (APS/Alan them imply a cause-effect relationship. John-Mark Allen at Stonebraker) the University of Oxford, UK, and colleagues have now pro- posed a quantum causal model based on a generalization of an old principle known as Reichenbach’s common cause is a third variable that is a common cause of both. In the principle [2]. latter case, the correlation will disappear if probabilities are Historically, statisticians thought that all information conditioned to the common cause. -
A WORLD WITHOUT CAUSE and EFFECT Logic-Defying Experiments Into Quantum Causality Scramble the Notion of Time Itself
A WORLD WITHOUT CAUSE AND EFFECT Logic-defying experiments into quantum causality scramble the notion of time itself. BY PHILIP BALL lbert Einstein is heading out for his This finding1 in 2015 made the quantum the constraints of a predefined causal structure daily stroll and has to pass through world seem even stranger than scientists had might solve some problems faster than con- Atwo doorways. First he walks through thought. Walther’s experiments mash up cau- ventional quantum computers,” says quantum the green door, and then through the red one. sality: the idea that one thing leads to another. theorist Giulio Chiribella of the University of Or wait — did he go through the red first and It is as if the physicists have scrambled the con- Hong Kong. then the green? It must have been one or the cept of time itself, so that it seems to run in two What’s more, thinking about the ‘causal struc- other. The events had have to happened in a directions at once. ture’ of quantum mechanics — which events EDGAR BĄK BY ILLUSTRATION sequence, right? In everyday language, that sounds nonsen- precede or succeed others — might prove to be Not if Einstein were riding on one of the sical. But within the mathematical formalism more productive, and ultimately more intuitive, photons ricocheting through Philip Walther’s of quantum theory, ambiguity about causation than couching it in the typical mind-bending lab at the University of Vienna. Walther’s group emerges in a perfectly logical and consistent language that describes photons as being both has shown that it is impossible to say in which way. -
Spin State Read-Out by Quantum Jump Technique
1 Spin State Read-Out by Quantum Jump Technique: for the Purpose of Quantum Computing E. Pazy Department of Physics, Ben-Gurion University of the Negev, Beer-Sheva 84105, Israel T. Calarco and P. Zoller Institut fur¨ Theoretische Physik, Universitat¨ Innsbruck, A-6020 Innsbruck, Austria Abstract—Utilizing the Pauli-blocking mechanism we in an isolated atom, self-assembled QDs are embedded show that shining circular polarized light on a singly in an underlying lattice ,i.e., a three-dimensional crystal charged quantum dot induces spin dependent fluorescence. structure. Even though the number of atoms in such Employing the quantum-jump technique we demonstrate dots is small compared to lithographically defined QDs, that this resonance luminescence, due to a spin dependent optical excitation, serves as an excellent read out mech- still this underlying lattice in which the QD is formed anism for measuring the spin state of a single electron strongly affects the single particle states through its band confined to a quantum dot. structure. Due to their discrete density of states, QDs have been I. INTRODUCTION suggested as the major building blocks for numerous quantum computing implementation schemes. These im- Semiconductor self-assembled quantum dots (QDs) plementation schemes can roughly be divided into those form spontaneously during the epitaxial growth process, which utilize the charge [2], or respectively the spin with confinement provided in all three dimensions by a [3] of charge carriers confined within a QD. Accurate high bandgap in the surrounding material (for example, measurement of a single qubit is an essential requirement see [1]). The strong confinement in such structures for the implementation of quantum computation (QC), leads to a discrete atom-like density of states which therefore highly precise methods for the measurement makes these QDs especially attractive for novel device arXiv:cond-mat/0404494v1 [cond-mat.other] 21 Apr 2004 of the spin of a QD confined charge carrier need to be applications in fields such as quantum computing, optics, devised. -
A Brief Introduction to Temporality and Causality
A Brief Introduction to Temporality and Causality Kamran Karimi D-Wave Systems Inc. Burnaby, BC, Canada [email protected] Abstract Causality is a non-obvious concept that is often considered to be related to temporality. In this paper we present a number of past and present approaches to the definition of temporality and causality from philosophical, physical, and computational points of view. We note that time is an important ingredient in many relationships and phenomena. The topic is then divided into the two main areas of temporal discovery, which is concerned with finding relations that are stretched over time, and causal discovery, where a claim is made as to the causal influence of certain events on others. We present a number of computational tools used for attempting to automatically discover temporal and causal relations in data. 1. Introduction Time and causality are sources of mystery and sometimes treated as philosophical curiosities. However, there is much benefit in being able to automatically extract temporal and causal relations in practical fields such as Artificial Intelligence or Data Mining. Doing so requires a rigorous treatment of temporality and causality. In this paper we present causality from very different view points and list a number of methods for automatic extraction of temporal and causal relations. The arrow of time is a unidirectional part of the space-time continuum, as verified subjectively by the observation that we can remember the past, but not the future. In this regard time is very different from the spatial dimensions, because one can obviously move back and forth spatially. -
K-Causal Structure of Space-Time in General Relativity
PRAMANA °c Indian Academy of Sciences Vol. 70, No. 4 | journal of April 2008 physics pp. 587{601 K-causal structure of space-time in general relativity SUJATHA JANARDHAN1;¤ and R V SARAYKAR2 1Department of Mathematics, St. Francis De Sales College, Nagpur 440 006, India 2Department of Mathematics, R.T.M. Nagpur University, Nagpur 440 033, India ¤Corresponding author E-mail: sujata [email protected]; r saraykar@redi®mail.com MS received 3 January 2007; revised 29 November 2007; accepted 5 December 2007 Abstract. Using K-causal relation introduced by Sorkin and Woolgar [1], we generalize results of Garcia-Parrado and Senovilla [2,3] on causal maps. We also introduce causality conditions with respect to K-causality which are analogous to those in classical causality theory and prove their inter-relationships. We introduce a new causality condition fol- lowing the work of Bombelli and Noldus [4] and show that this condition lies in between global hyperbolicity and causal simplicity. This approach is simpler and more general as compared to traditional causal approach [5,6] and it has been used by Penrose et al [7] in giving a new proof of positivity of mass theorem. C0-space-time structures arise in many mathematical and physical situations like conical singularities, discontinuous matter distributions, phenomena of topology-change in quantum ¯eld theory etc. Keywords. C0-space-times; causal maps; causality conditions; K-causality. PACS Nos 04.20.-q; 02.40.Pc 1. Introduction The condition that no material particle signals can travel faster than the velocity of light ¯xes the causal structure for Minkowski space-time. -
10. Light and Quantum Physics
10. Light and Quantum physics Infrared radiation Infrared is light that has a wavelength longer than that of visible light. It is often called “IR.” The longest wavelength visible light that we can see has a wavelength of about 0.65 microns. Infrared light has a wavelength from 0.65 microns up to about 20 microns. Since its wavelength is longer, its frequency is lower by the same factor. We humans emit infrared radiation because we are warm. The electrons in our atoms shake, since they are not at absolute zero. A shaking electron has a shaking electric field, and a shaking electric field emits an electromagnetic wave. The effect is analogous to the emission of all other waves: shake the ground enough, and you get an earthquake wave; shake water, and you get a water wave; shake the air, and you get sound; shake the end of a slinky, and a wave will travel along it. The result is that everything emits light, except things that have temperature at absolute zero. Everything glows -- but most things emit so little light, that we don't notice. And, of course we don't notice if most of the light is in a wavelength range that is invisible to the eye. What are some of the things that we notice when they glow from heat? Here are some: candle flame; anything being heated "red hot" in a flame; the sun; the tungsten filament of a 60-watt light bulb; an oven used for baking pottery. This glowing is often referred to as "thermal radiation" or as “heat radiation.” Thermal radiation and temperature The amount of thermal radiation can be calculated using the physics laws of thermodynamics. -
Location and Causality in Quantum Theory
Location and Causality in Quantum Theory A dissertation submitted to the University of Manchester for the degree of Master of Science by Research in the Faculty of Engineering and Physical Sciences 2013 Robert A Dickinson School of Physics and Astronomy Contents 1 Introduction 8 1.1 Causality . .8 1.2 Relativistic causality . .9 1.3 The structure of this document . 10 2 Correlations 12 2.1 Operational descriptions . 12 2.2 Restrictions on non-local correlations in a classical theory . 12 2.3 Parameter spaces of general correlations . 14 2.3.1 Imaginable parameter spaces for one binary observer . 15 2.3.2 One-way signalling between two observers . 15 2.3.3 Imaginable parameter spaces for two spacelike-separated binary observers . 17 2.3.4 The parameter space in nature for two spacelike-separated binary observers . 21 2.3.5 The parameter space in quantum theory for two spacelike- separated binary observers . 22 2.3.6 Parameter spaces for three or more spacelike-separated binary observers . 24 3 Hilbert Space 26 3.1 The Postulates and their implications . 26 3.2 Operational stochastic quantum theory . 28 3.2.1 Internal unknowns regarding the initial state . 29 3.2.2 External unknowns regarding the initial state . 30 3.2.3 Internal unknowns regarding the measurement . 30 3.2.4 External unknowns regarding the measurement . 31 3.2.5 The generalised update rule . 31 3.3 Causality in quantum mechanics . 33 3.3.1 The no-signalling condition . 33 3.3.2 Special cases . 35 3.4 From discrete to continuous sets of outcomes .